Optical system and imaging apparatus including the same

ABSTRACT

In an optical system in which a focal length of an entire system is shorter than a back focus, an image stabilizing lens unit, is at a position adjacent to an aperture on an image side and a cemented lens obtained by cementing a positive lens and a negative lens is on an object side of the aperture diaphragm, and the focal length of the entire system, a focal length of the image stabilizing lens unit, a focal length of the cemented lens, a distance on the optical axis from the aperture to a lens surface on the object side of the image stabilizing lens unit, and a distance on the optical axis from a first lens surface on a side closest to an object to a final lens surface on a side closest to an image when an infinite-distance object is brought into focus are set.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to an optical system and is suitable as animaging optical system used in an imaging apparatus such as asilver-halide film camera, a digital still camera, a video camera, adigital video camera, a monitoring camera, and a broadcasting camera,for example.

2. Description of the Related Art

It is required that the imaging optical system used in the imagingapparatus have high optical performance across an entire image area andthat various aberrations thereof be corrected in an excellent manner.The imaging optical system is also required to have an image stabilizingmechanism for inhibiting deterioration in image due to an effect ofvibration such as a camera shake at the time of shooting. As the imagestabilizing mechanism, a method of correcting variation in imageposition caused by the camera shake and the like by moving a part oflens units of the optical system in a direction including a componentperpendicular to the optical axis is known.

It is known that the image stabilizing mechanism is used in aretrofocus-type wide-angle lens in which a focal length of an entiresystem is shorter than a back focus.

In order to obtain excellent optical performance by correcting an imageshake at the time of vibration of the optical system, it is important toarrange the image stabilizing mechanism in an appropriate position ofthe imaging optical system.

U.S. Pat. No. 5,917,663 discloses that the wide-angle lens including alens unit with negative refractive power and a lens unit with positiverefractive power in order from an object side performs imagestabilization by rotational movement of two positive lenses on a sideclosest to an image around a point on the optical axis.

Therefore, an incident position of a principal ray of an off-axis rayincident on an image stabilizing lens unit becomes high and there is atendency that image-plane variation occurs at the time of the imagestabilization in the off-axis ray and aberration correction at the timeof the image stabilization becomes difficult. Also, the incident heightof the off-axis ray incident on the image stabilizing lens unit becomeshigh and there is a tendency that coma aberration variation becomeslarge at the time of the image stabilization and the optical performanceis deteriorated. Therefore, it is difficult to realize a large apertureratio of the wide-angle lens disclosed in U.S. Pat. No. 5,917,663.

In order to correct the image shake at the time of the vibration of theoptical system while maintaining the excellent optical performance, alens configuration and refractive power of the image stabilizing lensunit are important and it is also important to arrange the imagestabilizing lens unit at an appropriate position in an optical path.

An object of an embodiment of the present invention is to provide anoptical system capable of easily obtaining a high-quality image acrossthe entire image plane and of easily maintaining the excellent opticalperformance also at the time of the image stabilization with a wideangle of view and the large aperture ratio.

SUMMARY OF THE INVENTION

An optical system of an embodiment of the present invention is anoptical system of which a focal length of an entire system is shorterthan a back focus, wherein, when an image stabilizing lens unit, whichmoves in a direction including a component perpendicular to an opticalaxis to move an imaging position, is arranged at a position adjacent toan aperture diaphragm on an image side, a cemented lens obtained bycementing a positive lens and a negative lens is arranged on an objectside of the aperture diaphragm, the focal length of the entire system isset to f, a focal length of the image stabilizing lens unit is set tofis, a focal length of the cemented lens is set to fc, a distance on theoptical axis from the aperture diaphragm to a lens surface on the objectside of the image stabilizing lens unit is set to Dis, and a distance onthe optical axis from a first lens surface on a side closest to anobject to a final lens surface on a side closest to an image when aninfinite-distance object is brought into focus is set to DL, conditionequations

0.00<Dis/DL<0.25,

0.3<fis/f<3.5, and

0.3<−fc/fis<3.5

are satisfied.

Further features of the present invention will become apparent from thefollowing description of exemplary embodiments (with reference to theattached drawings).

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a cross-sectional view of a lens of a first embodiment;

FIG. 2 is a longitudinal aberration diagram of the first embodiment;

FIGS. 3A and 3B are lateral aberration diagrams in a reference state andat the time of 0.3° image stabilization correction of the firstembodiment of the present invention, respectively;

FIG. 4 is a cross-sectional view of a lens of a second embodiment;

FIG. 5 is a longitudinal aberration diagram of the second embodiment;

FIGS. 6A and 6B are lateral aberration diagrams in a reference state andat the time of 0.3° image stabilization correction of the secondembodiment of the present invention, respectively;

FIG. 7 is a cross-sectional view of a lens of a third embodiment;

FIG. 8 is a longitudinal aberration diagram of the third embodiment;

FIGS. 9A and 9B are lateral aberration diagrams in a reference state andat the time of 0.3° image stabilization correction of the thirdembodiment of the present invention, respectively;

FIG. 10 is a cross-sectional view of a lens of a fourth embodiment;

FIG. 11 is a longitudinal aberration diagram of the fourth embodiment;

FIGS. 12A and 12B are lateral aberration diagrams in a reference stateand at the time of 0.3° image stabilization correction of the fourthembodiment of the present invention, respectively; and

FIG. 13 is a schematic diagram of a substantial part of an imagingapparatus according to an embodiment of the present invention.

DESCRIPTION OF THE EMBODIMENTS

A preferred embodiment of the present invention is hereinafter describedin detail with reference to the attached drawings. In an optical systemof an embodiment of the present invention, a focal length of an entiresystem is shorter than a back focus. An image stabilizing lens unit,which moves in a direction including a component perpendicular to anoptical axis to move an imaging position, is arranged at a positionadjacent to an aperture diaphragm on an image side. A cemented lensobtained by cementing a positive lens and a negative lens is arranged onan object side of the aperture diaphragm.

FIG. 1 is a cross-sectional view of a lens of a first embodiment of thepresent invention and FIG. 2 is a longitudinal aberration diagram whenan infinite-distance object is brought into focus of the firstembodiment. FIGS. 3A and 3B are lateral aberration diagrams in areference state and at the time of 0.3° image stabilization correctionof the first embodiment of the present invention, respectively. FIG. 4is a cross-sectional view of a lens of a second embodiment of thepresent invention and FIG. 5 is a longitudinal aberration diagram whenan infinite-distance object is brought into focus of the secondembodiment. FIGS. 6A and 6B are lateral aberration diagrams in areference state and at the time of 0.3° image stabilization correctionof the second embodiment of the present invention, respectively.

FIG. 7 is a cross-sectional view of a lens of a third embodiment of thepresent invention and FIG. 8 is a longitudinal aberration diagram whenan infinite-distance object is brought into focus of the thirdembodiment. FIGS. 9A and 9B are lateral aberration diagrams in areference state and at the time of 0.3° image stabilization correctionof the third embodiment of the present invention, respectively. FIG. 10is a cross-sectional view of a lens of a fourth embodiment of thepresent invention and FIG. 11 is a longitudinal aberration diagram whenan infinite-distance object is brought into focus of the fourthembodiment. FIGS. 12A and 12B are lateral aberration diagrams in areference state and at the time of 0.3° image stabilization correctionof the fourth embodiment of the present invention, respectively. FIG. 13is a schematic diagram of a substantial part of a single-lens reflexcamera (imaging apparatus) provided with the optical system in anembodiment of the present invention.

The optical system of each embodiment is an imaging optical system usedin the imaging apparatus (optical apparatus) such as a digital stillcamera, a video camera, and a silver-halide film camera. In thecross-sectional view of the lens, a left side is the object side (frontside) and a right side is the image side (rear side). Meanwhile, theoptical system of each embodiment may also be used as a projection lensof a projector and the like. At that time, the left side is a screen andthe right side is an image to be projected.

In the cross-sectional view of the lens, a reference sign LA representsthe optical system. The optical system LA includes a front lens unit LFon the object side and a rear lens unit LR with positive refractivepower on the image side across an aperture diaphragm SP. Reference signsL1 and L2 represent a first lens unit with positive or negativerefractive power, which does not move during focusing, and a second lensunit with positive refractive power, which moves during focusing,respectively.

The second lens unit L2 includes a lens unit on each of the object sideand the image side of the aperture diaphragm (diaphragm) SP. The secondlens unit L2 includes an image stabilizing lens unit Gis including asingle lens or a cemented lens at the position adjacent to the aperturediaphragm SP on the image side. A reference sign Lc represents thecemented lens with negative refractive power arranged on the object sideof the image stabilizing lens unit Gis. A reference sign IP representsan image plane, which corresponds to an image sensing plane of asolid-state image sensing device (photoelectric transducer) such as aCCD sensor and a CMOS sensor when the imaging optical system is used asthat of the video camera and the digital still camera and corresponds toa film plane when this is used in the silver-halide film camera.

Each longitudinal aberration diagram illustrates a spherical aberration,astigmatism, a distortion, and a magnification chromatic aberration inorder from left to right. In the diagrams, which illustrate thespherical aberration and the magnification chromatic aberration, a solidline indicates a d-line (587.6 nm) and a broken line indicates a g-line(435.8 nm). In the diagram, which illustrates the astigmatism, a solidline S indicates a sagittal direction of the d-line and a broken line Mindicates a meridional direction of the d-line. The diagram, whichillustrates the distortion, illustrates the distortion in the d-line. Inthe lateral aberration diagram, a solid line, a broken line, and atwo-dot chain line indicate the meridional direction of the d-line, thesagittal direction of the d-line, and the meridional direction of theg-line, respectively. Reference signs Fno, ω, and hgt represent anF-number, a half angle of view (degree) of an angle of view forshooting, and an image height, respectively.

A specific configuration of the optical system of an embodiment of thepresent invention is an imaging optical system including the first lensunit L1 with positive or negative refractive power and the second lensunit L2 with positive refractive power in order from the object side tothe image side. The imaging optical system performs focusing by movingthe second lens unit L2 on the optical axis. The first lens unit L1includes a negative lens in a meniscus shape having a convex surface onthe object side and a positive lens having a surface in a convex shapeon the object side in order from the object side to the image side. Thesecond lens unit L2 includes a lens with negative refractive power(negative lens) in the meniscus shape having a concave surface on theimage side, a lens with positive refractive power (positive lens), thecemented lens with negative refractive power obtained by cementing thepositive lens and the negative lens, and the aperture diaphragm in orderfrom the object side to the image side.

The second lens unit L2 further includes the image stabilizing lens unitGis with positive refractive power, which reduces an image shake bymoving in the direction including the component in the directionperpendicular to the optical axis, a cemented lens obtained by cementinga negative lens and a positive lens, and a positive lens on the imageside of the aperture diaphragm SP.

In general, in the imaging optical system, a height of an off-axis rayat a maximum angle of view from the optical axis is higher as a distancefrom the aperture diaphragm SP in an optical axis direction is larger.Therefore, an effective ray diameter of the lens arranged at a positionapart from the aperture diaphragm SP becomes larger. Therefore, when theimage stabilizing lens unit Gis is arranged in the vicinity of theaperture diaphragm SP, the effective ray diameter thereof becomessmaller and a small lens diameter may be easily realized even whenmovement for image stabilization is taken into account. Since anincident height of a ray, which passes through the image stabilizinglens unit Gis, is low, aberration variation at the time of the imagestabilization may easily be made small.

Therefore, in the optical system of each embodiment, the imagestabilizing lens unit is arranged in a position near the aperturediaphragm SP as described above for inhibiting an effective diameter ofthe image stabilizing lens unit from becoming large. As a result, a loadon a driving mechanism of the image stabilizing lens is decreased and anentire lens may be made compact easily. At the same time, the lens unitat the position near the aperture diaphragm SP in an entire system ismade the image stabilizing lens unit, which moves in the directionincluding the component in the direction perpendicular to the opticalaxis. According to this, the optical system in which the height of theoff-axis ray, which passes through the image stabilizing lens unit, islow and the aberration variation of the off-axis ray at the time of theimage stabilization is small is realized.

Especially, when a large aperture is realized, a lens diameter of theoptical system becomes larger and the lens diameter of the imagestabilizing lens unit also becomes larger. The image stabilizing lensunit becomes heavier along with the increase in lens diameter and animage stabilizing driving mechanism becomes further larger. When thelarge aperture is realized, a light-weight image stabilizing lens unitis preferable and the number of lenses is desirably made small. However,when the large aperture is realized, a diameter of luminous flux of theon-axis ray becomes larger and optical performance is deteriorated dueto coma aberration variation at the time of the image stabilization.

For the above-described reason, in the imaging optical system, it isimportant to efficiently cancel out the aberration occurring in theimage stabilizing lens unit Gis including a small number of lenses byanother lens unit such that the aberration may be sufficiently correctedalso at the time of the image stabilization using a small number oflenses. Therefore, in the optical system of each embodiment, thecemented lens Lc with negative refractive power as a whole obtained bycementing the lens with positive refractive power and the lens withnegative refractive power as a supplementary lens unit is arranged onthe object side of the image stabilizing lens unit Gis.

According to this, sufficient aberration correction may be performedeven with a small number of lenses. Since the image stabilizing lensunit Gis includes one lens (image stabilizing lens), the imagestabilizing lens unit Gis is not excessively heavy also when a largeaperture ratio is realized and it becomes easy to compose the imagestabilizing lens unit without a large burden on the image stabilizingdriving mechanism. Since the refractive power with different signs isapplied to the image stabilizing lens unit Gis and the supplementarylens unit Lc adjacent to the same in this manner, it becomes easy toapply appropriate image shaking sensitivity to the image stabilizinglens unit Gis.

In each embodiment, the image stabilizing lens unit Gis is displaced ina direction including a component perpendicular to the optical axis forthe image stabilization to correct the image shake caused by vibrationsuch as a camera shake. Herein, the “direction including the componentin the direction orthogonal to the optical axis” includes not only adirection orthogonal to the optical axis but also a direction shiftedfrom the direction orthogonal to the optical axis (for example, adirection inclined with respect to the direction orthogonal to theoptical axis and a rotation direction around a point on the opticalaxis).

In each embodiment, the focal length of the entire system is set to f,the focal length of the image stabilizing lens unit Gis is set to fis,and the focal length of the cemented lens Lc is set to fc. A distance onthe optical axis from the aperture diaphragm SP to a lens surface on anaperture diaphragm SP side of the image stabilizing lens unit Gis is setto Dis and the distance on the optical axis from a first lens surface onthe object side to a final lens surface when the infinite-distanceobject is brought into focus is set to DL. At that time, conditionequations

0.00<Dis/DL<0.25  (1),

0.3<fis/f<3.5  (2), and

0.3<−fc/fis<3.5  (3)

are satisfied.

Herein, the “distance on the optical axis” in a direction from theobject side to the image side is with a positive sign and that in anopposite direction (direction from the image side to the object side) iswith a negative sign.

Next, a technical meaning of each condition equation described above isdescribed. The condition equation (1) represents a condition forrealizing an appropriate distance on the optical axis from the aperturediaphragm SP to the lens surface closest to the aperture diaphragm SP ofthe image stabilizing lens unit Gis.

When the image stabilizing lens unit Gis is too much away from theaperture diaphragm SP toward the image side beyond an upper limit of thecondition equation (1), the effective diameter of the image stabilizinglens unit Gis adversely increases. The incident height of the off-axisray, which passes through the image stabilizing lens unit Gis, from theoptical axis also becomes higher, so that the aberration correction ofthe off-axis ray at the time of the image stabilization becomesdifficult. When the image stabilizing lens unit Gis gets so closer tothe aperture diaphragm SP as to approach a lower limit of the conditionequation (1), interference between the aperture diaphragm SP and theimage stabilizing lens unit Gis adversely easily occurs. Meanwhile, anumerical range of the condition equation (1) is more preferably set asfollows:

0.00<Dis/DL<0.07  (1a).

The condition equation (2) is the condition equation for maintainingsensitivity in aberration variation and sensitivity in displacement ofan image position in a balanced manner when the image stabilizing lensunit Gis is displaced in the direction perpendicular to the optical axisby realizing an appropriate ratio of the focal length of the imagestabilizing lens unit Gis to the focal length of the entire system. Whenthe refractive power of the image stabilizing lens unit Gis becomesweaker beyond the upper limit of the condition equation (2), an amountof movement in the direction including the component in the directionperpendicular to the optical axis becomes larger at the time of theimage stabilization, so that the driving mechanism becomes larger.

When the refractive power of the image stabilizing lens unit Gis becomesstronger beyond the lower limit of the condition equation (2), a largeeccentric aberration occurs at the time of the image stabilization andthe optical performance at the time of the image stabilization isadversely deteriorated. An amount of change of the image position withrespect to an amount of displacement of the image stabilizing lens unitGis (hereinafter, referred to as the image shaking sensitivity) becomeslarge, so that the amount of displacement of the image stabilizing lensunit Gis for obtaining a required image stabilization effect becomes toosmall and it becomes difficult to electrically or mechanically controlthe amount of displacement at high accuracy. The numerical range of thecondition equation (2) is further preferably set as follows:

0.5<fis/f<3.0  (2a).

The condition equation (3) is for appropriately setting refractive powerbalance between the image stabilizing lens unit Gis and the cementedlens (supplementary lens) Lc obtained by cementing the lens withpositive refractive power and the lens with negative refractive power onthe object side thereof. This is especially the condition equation formaintaining appropriate balance between aberration correction share andsensitivity in image position correction when the image stabilizing lensunit Gis is displaced in the direction perpendicular to the opticalaxis. In each embodiment, the cemented lens Lc is arranged on the objectside of the image stabilizing lens unit Gis for inhibiting an axialchromatic aberration, which occurs when the appropriate refractive powerbalance is realized.

When the refractive power of the image stabilizing lens unit Gis becomesstronger beyond the upper limit of the condition equation (3), thelarger eccentric aberration occurs at the time of the imagestabilization and the optical performance is deteriorated. When therefractive power of the image stabilizing lens unit Gis becomes weakerbeyond the lower limit of the condition equation (3), the image shakingsensitivity becomes too low and the amount of drive in the directionincluding the component perpendicular to the optical axis becomes largerat the time of the image stabilization, so that the driving mechanismbecomes adversely larger. The numerical range of the condition equation(3) is further preferably set as follows:

0.5<−fc/fis<3.0  (3a).

In each embodiment, the above-described conditions are satisfied forobtaining a wide-view-angle lens, which makes it easy to obtain acompact image stabilizing lens unit Gis and makes it possible to obtainan excellent image also at the time of the image stabilization with thehigh optical performance. Also, in each embodiment, the lens withpositive refractive power having an aspherical surface is preferablyarranged on a side closest to the image plane. By arranging the lenswith positive refractive power having an aspherical surface shape on aside closest to the image, tilt of a sagittal image plane may be reducedand it becomes easy to obtain the excellent optical performance also onthe periphery of an image plane.

In each embodiment, one or more of following condition equations isdesirably satisfied in order to obtain the high optical performancewhile maintaining the excellent optical performance at the time of theimage stabilization. Lateral magnification of the image stabilizing lensunit Gis is set to βis and the lateral magnification of the lens unitarranged on the image side of the image stabilizing lens unit Gis is setto βr. The image stabilizing lens unit Gis includes the single lens andan Abbe number of a material of the single lens with respect to thed-line is set to νdis. At that time, one or more of the followingcondition equations is preferably satisfied:

0.1<|(1−βis)βr|<1.3  (4) and

35<νdis  (5).

The condition equation (4) relates to a ratio between the amount ofmovement of the image stabilizing lens unit Gis in the directionperpendicular to the optical axis and an image point moving amount on animaging plane generated according to this, and the larger this value is,the smaller the amount of movement for large and easy movement of theimage point is. Hereinafter, a value of the condition equation (4) isreferred to as the image shaking sensitivity.

When the image shaking sensitivity is too high beyond the upper limit ofthe condition equation (4), the amount of displacement (amount ofmovement) of the image stabilizing lens unit Gis for obtaining a certainimage stabilization effect becomes too small and electrical ormechanical drive for the amount of movement at high accuracy becomesdifficult. When the image shaking sensitivity is too low beyond thelower limit of the condition equation (4), the amount of movement so asto include the component in the direction perpendicular to the opticalaxis at the time of the image stabilization becomes larger and thedriving mechanism adversely becomes larger. The numerical range of thecondition equation (4) is further preferably set as follows:

0.2<|(1−βis)βr|<1.0  (4a).

The condition equation (5) relates to the Abbe number of the material ofthe image stabilizing lens, which composes the image stabilizing lensunit Gis, with respect to the d-line and is the condition equation forcorrecting especially a chromatic aberration such as the axial chromaticaberration and the magnification chromatic aberration out of theaberrations occurring at the time of the image stabilization in anexcellent manner.

The image stabilizing lens unit Gis desirably includes as few lenses aspossible for downsizing and weight saving. The image stabilizing lensunit Gis most preferably includes one positive lens or one negativelens. That is, the image stabilizing lens unit Gis most preferablyincludes the single lens. When the Abbe number of the material, whichcomposes the image stabilizing lens unit Gis, is small beyond the lowerlimit of the condition equation (5), the chromatic aberration such asthe axial chromatic aberration and the magnification chromaticaberration occurring at the time of the image stabilization becomeslarge and it becomes difficult to correct them. The numerical range ofthe condition equation (5) is further preferably set as follows:

40<νdis  (5a).

As described above, according to each embodiment, a so-calledretrofocus-type optical system in which the focal length of the entiresystem is shorter than the back focus having the excellent opticalperformance without large various aberrations occurring at the time ofthe image stabilization is obtained. At the same time, a compact opticalsystem having a simple lens configuration in which an excessive loaddoes not occur in the mechanism for driving the image stabilizing lensunit is easily obtained.

Next, an embodiment of a single-lens reflex camera system (imagingapparatus) in which the optical system of an embodiment of the presentinvention is used is described with reference to FIG. 13. In FIG. 13,reference numerals 10 and 11 represent a single-lens reflex camera mainbody and an interchangeable lens equipped with the optical systemaccording to an embodiment of the present invention, respectively. Areference numeral 12 represents a recording unit such as a film and animage sensing device for recording a subject image obtained through theinterchangeable lens 11. Reference numerals 13 and 14 represent aviewfinder optical system for observing the subject image from theinterchangeable lens 11 and a quick-return mirror, which rotates, fortransmitting the subject image formed by the interchangeable lens 11 tothe recording unit 12 and the viewfinder optical system 13 in aswitching manner.

When the subject image is observed in the viewfinder, the subject imageformed on a focusing plate 15 through the quick-return mirror 14 is madean erect image by a pentagonal prism 16 and enlarged to be observed byan eyepiece optical system 17. At the time of shooting, the quick-returnmirror 14 rotates in a direction indicated by an arrow and the subjectimage is formed on the recording unit 12 to be recorded. Referencenumerals 18 and 19 represent a sub mirror and a focus detecting unit,respectively. It is possible to realize the imaging apparatus having thehigh optical performance by applying the optical system of an embodimentof the present invention to the imaging apparatus such as theinterchangeable lens of the single-lens reflex camera and the like inthis manner. Meanwhile, the optical system of an embodiment of thepresent invention may also be applied to a mirrorless camera without thequick-return mirror.

First to fourth numerical embodiments corresponding to the first tofourth embodiments, respectively, are hereinafter described. In eachnumerical embodiment, reference signs i and ri represent an order ofsurfaces from the object side and a curvature radius of i-th one (i-thsurface), respectively. A reference sign di represents an intervalbetween the i-th surface and an (i+1)-th surface. Reference signs ndiand νdi represent a refractive index and the Abbe number based on thed-line, respectively. A reference sign BF represents the back focus. Thesurface with a mark * is the aspherical surface. (Aspherical surfacedata) indicates an aspherical surface coefficient when the asphericalsurface is represented by an equation

x=(h ² /R)/[1+{1−(1+k)(h/R)²}^(1/2) +A4·h ⁴ +A6·h ⁶ +A8·h ⁸ +A10·h ¹⁰+A12·h ¹²,

whereinx represents an amount of displacement from a reference plane in theoptical axis direction,h represents a height in the direction perpendicular to the opticalaxis, andR represents a radius of a secondary curved surface, which is a base.

Reference signs A4, A6, A8, A10, and A12 are fourth-order, sixth-order,eighth-order, tenth-order, and twelfth-order aspherical surfacecoefficients, respectively. Meanwhile, representation “e-Z” is intendedto mean “10^(−z)”. A relationship between each of the above-describedcondition equations and various values in the numerical embodiments isindicated in table 1.

First Numerical Embodiment

unit: mm Surface Data surface number r d nd νd  1 107.841 2.00 1.4874970.2  2 36.325 3.37  3 60.900 4.53 1.77250 49.6  4 253.393 9.91  5478.362 1.50 1.58144 40.8  6 19.063 9.05  7 32.422 4.55 1.88300 40.8  8−98.623 3.98  9 −54.460 3.64 1.88300 40.8 10 −20.463 1.00 1.61293 37.011 63.422 3.24 12 (diaphragm) ∞ 2.68 13 69.180 2.29 1.69680 55.5 14−128.073 5.46 15 −15.746 0.95 1.73800 32.3 16 −131.434 4.37 1.59522 67.717 −18.862 0.20 18* −91.820 3.48 1.58313 59.4 19 −23.365 AsphericalSurface Data 18th surface K = 0.00000e+000 A 4 = −1.49529e−005 A 6 =4.91763e−009 A 8 = −4.11063e−011 focal length 34.49 F number 2.05 halfangle of view (degree) 32.10 image height 21.64 total lens length 104.50BF 38.30

Second Numerical Embodiment

unit: mm Surface Data surface number r d nd νd  1 132.460 2.00 1.6229958.2  2 34.266 4.76  3 93.710 4.21 1.77250 49.6  4 −524.055 9.95  568.381 1.50 1.60562 43.7  6 22.966 7.04  7 27.744 6.32 1.83481 42.7  8−106.109 2.76  9 −52.472 3.53 1.83400 37.2 10 −23.397 1.10 1.59551 39.211 36.125 3.72 12 (diaphragm) ∞ 2.35 13 72.096 2.30 1.72916 54.7 14−124.797 5.65 15 −14.420 1.00 1.78472 25.7 16 −102.223 3.96 1.83481 42.717 −20.023 0.20 18* −58.818 4.29 1.58313 59.4 19 −20.458 AsphericalSurface Data 18th surface K = 0.00000e+000 A 4 = −1.82729e−005 A 6 =3.11467e−008 A 8 = −5.17296e−010 A10 = 2.93372e−012 A12 = -5.92984e−015focal length 34.49 F number 2.02 half angle of view (degree) 32.10 imageheight 21.64 total lens length 104.24 BF 37.58

Third Numerical Embodiment

unit: mm Surface Data surface number r d nd νd  1 71.195 2.00 1.4874970.2  2 36.050 3.76  3 63.886 4.12 1.77250 49.6  4 221.701 11.17  5−214.904 1.50 1.58144 40.8  6 19.706 8.54  7 37.566 4.39 1.88300 40.8  8−77.437 4.20  9 −49.840 3.75 1.88300 40.8 10 −19.588 1.00 1.60342 38.011 202.255 2.40 12 (diaphragm) ∞ 2.64 13 98.946 1.79 1.72916 54.7 14−203.419 5.7 15 −15.432 0.95 1.68893 31.1 16 −78.954 4.52 1.49700 81.517 −17.330 0.20 18* −104.072 3.57 1.58313 59.4 19 −23.339 AsphericalSurface Data 18th surface K = 0.00000e+000 A 4 = −1.57839e−005 A 6 =8.94837e−009 A 8 = −5.94828e−011 focal length 34.5 F number 2.05 halfangle of view (degree) 32.09 image height 21.64 total lens length 104.5BF 38.3

Fourth Numerical Embodiment

unit: mm Surface Data surface number r d nd νd  1 156.683 2.00 1.4874970.2  2 39.154 3.56  3 75.419 4.65 1.77250 49.6  4 −24596.307 10.41  5−220.720 1.50 1.58144 40.8  6 19.974 7.76  7 32.644 4.39 1.88300 40.8  8−112.408 4.77  9 −61.668 3.78 1.88300 40.8 10 −20.465 1.00 1.62004 36.311 114.664 2.62 12 (diaphragm) ∞ 2.52 13 74.645 2.15 1.72916 54.7 14−129.232 5.32 15 −16.296 0.95 1.73800 32.3 16 −293.682 5.27 1.59522 67.717 −20.362 0.20 18* −67.364 3.35 1.58313 59.4 19 −22.066 AsphericalSurface Data 18th surface K = 0.00000e+000 A 4 = −1.61559e−005 A 6 =3.74810e−009 A 8 = −5.07547e−011 focal length 34.47 F number 2.05 halfangle of view (degree) 32.11 image height 21.64 total lens length 104.5BF 38.3

TABLE 1 Condition First Second Third Fourth equations embodimentembodiment embodiment embodiment (1) 0.040 0.035 0.040 0.038 (2) 1.881.83 2.65 1.89 (3) 1.23 0.71 1.81 2.30 (4) 0.614 0.603 0.432 0.613 (5)55.5 54.7 54.7 54.7

While the present invention has been described with reference toexemplary embodiments, it is to be understood that the invention is notlimited to the disclosed exemplary embodiments. The scope of thefollowing claims is to be accorded the broadest interpretation so as toencompass all such modifications and equivalent structures andfunctions.

This application claims the benefit of Japanese Patent Application No.2012-072806, filed Mar. 28, 2012, which is hereby incorporated byreference herein in its entirety.

What is claimed is:
 1. An optical system of which a focal length of anentire system is shorter than a back focus, wherein, when an imagestabilizing lens unit, which moves in a direction including a componentperpendicular to an optical axis to move an imaging position, isarranged at a position adjacent to an aperture diaphragm on an imageside, a cemented lens obtained by cementing a positive lens and anegative lens is arranged on an object side of the aperture diaphragm,the focal length of the entire system is set to f, a focal length of theimage stabilizing lens unit is set to fis, a focal length of thecemented lens is set to fc, a distance on the optical axis from theaperture diaphragm to a lens surface on the object side of the imagestabilizing lens unit is set to Dis, and a distance on the optical axisfrom a first lens surface on a side closest to an object to a final lenssurface on a side closest to an image when an infinite-distance objectis brought into focus is set to DL, condition equations0.00<Dis/DL<0.25,0.3<fis/f<3.5, and0.3<−fc/fis<3.5 are satisfied.
 2. The optical system according to claim1, wherein, when lateral magnification of the image stabilizing lensunit is set to βis and lateral magnification of a lens unit arranged onthe image side of the image stabilizing lens unit is set to βr, acondition equation0.1<|(1−βis)βr|<1.3 is satisfied.
 3. The optical system according toclaim 1, wherein, when the image stabilizing lens unit includes a singlelens and an Abbe number of a material of the single lens with respect toa d-line is set to νdis, a condition equation35<νdis is satisfied.
 4. The optical system according to claim 1,comprising: a first lens unit with positive or negative refractive powerand a second lens unit with positive refractive power in order from theobject side to the image side, wherein the second lens unit moves duringfocusing, and the cemented lens, the aperture diaphragm, and the imagestabilizing lens unit are included in the second lens unit.
 5. Theoptical system according to claim 4, wherein the first lens unitincludes a negative lens in a meniscus shape having a convex surface onthe object side and a positive lens in order from the object side to theimage side, and the second lens unit includes a negative lens in themeniscus shape having a concave surface on the image side, a positivelens, the cemented lens obtained by cementing the positive lens and thenegative lens, the aperture diaphragm, the image stabilizing lens unit,which moves in the direction including the component in the directionperpendicular to the optical axis to move the imaging position, acemented lens obtained by cementing a negative lens and a positive lens,and a positive lens in order from the object side to the image side. 6.The optical system according to claim 1, wherein the lens on the sideclosest to the image is a positive lens having an aspherical surface. 7.An imaging apparatus, comprising: the optical system according to claim1.